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Publication numberUS7688525 B2
Publication typeGrant
Application numberUS 11/654,131
Publication dateMar 30, 2010
Filing dateJan 17, 2007
Priority dateJan 17, 2006
Fee statusPaid
Also published asCN101375112A, EP1994336A2, US20070188876, WO2007084518A2, WO2007084518A3
Publication number11654131, 654131, US 7688525 B2, US 7688525B2, US-B2-7688525, US7688525 B2, US7688525B2
InventorsBraden E. Hines, Richard L. Johnson, JR.
Original AssigneeSoliant Energy, Inc.
Export CitationBiBTeX, EndNote, RefMan
External Links: USPTO, USPTO Assignment, Espacenet
Hybrid primary optical component for optical concentrators
US 7688525 B2
Abstract
A hybrid optical component that collects and concentrates incident light. The hybrid component includes both refractive and reflective elements. In preferred embodiments, refractive and reflective components focus rays on a common focal plane generally located at the bottom of the reflector where they are absorbed by a device such as a photovoltaic (solar) cell. Additionally, the optical component combines both imaging and non-imaging optical elements into a single device, for improved overall performance.
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Claims(38)
1. A hybrid, concentrating optical component, comprising:
i. an aperture;
ii. a reflective optical element that collects and focuses light onto a first target for a first portion of the aperture; and
iii. a refractive optical element that collects and focuses light onto a second target for a second portion of the aperture,
wherein at least one of the first and second targets is an aperture of one or more secondary optics.
2. The hybrid concentrating optical component of claim 1, wherein the first and second targets are the same.
3. The hybrid concentrating optical component of claim 1, wherein the first and second targets comprise a portion of a common focal plane.
4. The hybrid concentrating optical component of claim 3, wherein the common focal plane is proximal to a bottom focus of the optical system.
5. The hybrid concentrating optical component of claim 1, wherein the component concentrates light onto a line.
6. The hybrid concentrating optical component of claim 1, wherein the component concentrates light onto a point.
7. The hybrid concentrating optical component of claim 1, wherein the component is a constituent of a system that is self powered.
8. The hybrid concentrating optical component of claim 1, wherein the component is a constituent of a system that includes a plurality of articulating modules, said optical component concentrating light for at least one of said modules.
9. The hybrid concentrating optical component of claim 1, wherein the reflective element is a bottom focusing, reflective dish.
10. The hybrid concentrating optical component of claim 1, wherein the reflective element is a bottom focusing reflective trough.
11. A hybrid, concentrating optical component, comprising:
i. an aperture;
ii. a reflective optical element that collects and focuses light onto a first target for a first portion of the aperture; and
iii. a refractive optical element that collects and focuses light onto a second target for a second portion of the aperture, wherein the refractive element comprises a fresnel lens.
12. The hybrid concentrating optical component of claim 11, wherein the fresnel lens concentrates light onto a line.
13. The hybrid concentrating optical component of claim 11, wherein the fresnel lens concentrates light onto a point.
14. The hybrid concentrating optical component of claim 1, wherein the refractive optical clement and the reflective optical element have a common optical axis.
15. The hybrid concentrating optical component of claim 14, wherein the refractive element is centered upon the common optical axis.
16. The hybrid concentrating optical component of claim 2, wherein the component comprises an aperture region associated with reflected light that passed through said aperture region and that is non-absorbed by the target, and wherein the refractive optical element is positioned in a manner effective to cause refracted light that passes through said aperture region to be absorbed by the target.
17. The hybrid concentrating optical component of claim 1, wherein a cover fits over a light receiving end of the reflective optical component, said cover incorporating the refractive optical element.
18. The hybrid concentrating optical component of claim 1, wherein the refractive element is positioned in a portion of the aperture that is unusable by the reflective element for concentration.
19. The hybrid concentrating optical component of claim 1, wherein the refractive element is a lens.
20. The hybrid concentrating optical component of claim 1, wherein the refractive element is a fresnel lens.
21. The hybrid concentrating optical component of claim 1, wherein the reflective element is a reflecting surface that has a geometry selected from a linear, parabolic, spherical, elliptical, and hyperbolic profile.
22. A hybrid, concentrating optical component, comprising:
i. an aperture;
ii. a reflective optical element that collects and focuses light onto a first target for a first portion of the aperture. wherein said reflective optical element comprises first and second reflective optical elements, each element collecting and concentrating incident light for respective portions of the first portion of the aperture; and
iii. a refractive optical element that collects and focuses light onto a second target for a second portion of the aperture.
23. A hybrid, concentrating optical component, comprising:
i. an aperture;
ii. a reflective optical element that collects and focuses light onto a first target for a first portion of the aperture, wherein the reflective optical element comprises a plurality of facets; and
iii. a refractive optical element that collects and focuses light onto a second target for a second portion of the aperture.
24. A hybrid, concentrating optical component, comprising:
i. an aperture;
ii. a reflective optical element that collects and focuses light onto a first target for a first portion of the aperture;
iii. a refractive optical element that collects and focuses light onto a second target for a second portion of the aperture; and
iv. a path for diffuse radiation to reach a target surface.
25. The hybrid concentrating optical component of claim 24, wherein the optical path for diffuse radiation impinges on the target surface without being reflected onto the target surface.
26. The hybrid concentrating optical component of claim 25, wherein the optical path for diffuse radiation impinges on the target surface without being refracted onto the target surface.
27. The hybrid concentrating optical component of claim 11, wherein the first and second targets are the same.
28. The hybrid concentrating optical component of claim 11, wherein a cover fits over a light receiving end of the reflective optical component, said cover incorporating the refractive optical element.
29. The hybrid concentrating optical component of claim 11, wherein the refractive element is positioned in a portion of the aperture that is unusable by the reflective element for concentration.
30. The hybrid concentrating optical component of claim 22, wherein the first and second targets are the same.
31. The hybrid concentrating optical component of claim 22, wherein a cover fits over a light receiving end of the reflective optical component, said cover incorporating the refractive optical element.
32. The hybrid concentrating optical component of claim 22, wherein the refractive element is positioned in a portion of the aperture that is unusable by the reflective element for concentration.
33. The hybrid concentrating optical component of claim 23, wherein the first and second targets are the same.
34. The hybrid concentrating optical component of claim 23, wherein a cover fits over a light receiving end of the reflective optical component, said cover incorporating the refractive optical element.
35. The hybrid concentrating optical component of claim 23, wherein the refractive element is positioned in a portion of the aperture that is unusable by the reflective element for concentration.
36. The hybrid concentrating optical component of claim 24, wherein the first and second targets are the same.
37. The hybrid concentrating optical component of claim 24, wherein a cover fits over a light receiving end of the reflective optical component, said cover incorporating the refractive optical element.
38. The hybrid concentrating optical component of claim 24, wherein the refractive element is positioned in a portion of the aperture that is unusable by the reflective element for concentration.
Description
PRIORITY CLAIM

The present non-provisional patent Application claims priority under 35 USC §119(e) from U.S. Provisional Patent Application having Ser. No. 60/759,909, filed on Jan. 17, 2006, by Hines et al., and titled A HYBRID PRIMARY OPTICAL COMPONENT FOR OPTICAL CONCENTRATORS, wherein the entirety of said provisional patent application is incorporated herein by reference.

FIELD OF THE INVENTION

This invention relates to optical configurations applied to optical concentrating systems, such as line or point solar collectors that receive and concentrate incident light towards target(s). The target(s) may be device(s) such as photovoltaic (solar) cell(s).

BACKGROUND OF THE INVENTION

Optical concentrating systems, such as solar collectors, concentrate light toward a focus of the optical system. In general, there are two categories of concentrators. Line concentrators concentrate incident light in one dimension so that the focus is a line. Point concentrators concentrate incident light in two dimensions so that the focus is a point.

Concentrators may include one or more optical components to concentrate incident light. Some systems have a single concentrating optical component, referred to as the primary optic, that concentrates rays directly onto the desired target (which may be a device such as a photovoltaic cell) after being collected and focused by the optic. More complex concentrators may include both a primary optic and additional optics to provide further collection or concentration abilities or improve beam uniformity at the target.

A primary optic for an optical concentrator typically includes either a refractive component or a reflective component. The most common refractive component employed is a Fresnel lens, as in O'Neill, U.S. Pat. No. 4,069,812, while a common reflective component is a parabolic reflector. With respect to refractive components, Fresnel lenses are usually preferred over standard lenses, because Fresnel lenses are thinner for a given aperture. As such, Fresnel lenses allow large collecting apertures without requiring as much lens material as does a standard lens. The system aperture for these concentrators is defined by the aperture of the Fresnel lens. FIG. 2 illustrates a typical Fresnel lens concentrator having optical axis 24, showing a Fresnel lens 18 bending light rays 20 towards a desired focus 16.

Large, high quality Fresnel lenses as conventionally used, however, can be prohibitively expensive for medium scale applications such as commercial rooftop systems. In addition, surface discontinuities present on Fresnel lenses tend to make them lossy (i.e., inasmuch as some of the light that is desirably focused may instead be absorbed and/or directed away from the focus) compared to standard lenses or reflective solutions. Another disadvantage of the Fresnel concentrator as conventionally used is that it is not suitable by itself for certain articulating concentrators that require self-powering. Such devices require a means to generate power when the optical axis of the concentrator is not aligned with the sun thereby relying on diffuse radiation from the sky. Unfortunately, a conventional Fresnel concentrator provides negligible paths for diffuse radiation to strike a solar cell located at the focus of the lens and therefore is usually unable to generate sufficient power to articulate itself when not aligned with the sun.

Reflective primaries are known to include compound parabolic concentrators (CPCs) as per Winston, U.S. Pat. No. 4,003,638 well as various types of parabolic or nearly parabolic troughs and dishes. CPCs provide good beam uniformity at the focal plane. Troughs and dishes are the two main types of CPC's. Troughs and dishes may have a bottom focus wherein the optical target, for example a solar cell, is facing up. Troughs and dishes with a bottom focus advantageously may collect and concentrate diffuse light even when the reflector is not directly aimed at the source(s) of the diffuse light. This makes them suitable for collecting diffuse light used for self-power. Troughs and dishes also may have an inverted focus wherein the optical target, for example a solar cell, is facing down, often suspended above the reflector.

However, because high concentration ratios tend to require a CPC with a large height/width ratio, the packing density for multiple articulating concentrators including CPC's can be limited. For example, FIG. 3 of the present application schematically illustrates a typical bottom focus CPC 28 with a geometric concentration of 10× in one dimension. Incident rays 30 are concentrated onto focal plane 26 with a normalized width of 1. The normalized height of the CPC 28 is 17.8, resulting in a height/width ratio of 1.78.

This relatively high height/width ratio factor makes conventional CPC's, by themselves, poorly suited for multiple articulating concentrator systems such as those described in Assignee's U.S. Provisional Patent Application No. 60/691,319, filed Jun. 16, 2005, in the names of Hines et al., titled PLANAR CONCENTRATING PHOTOVOLTAIC SOLAR PANEL WITH INDIVIDUALLY ARTICULATING CONCENTRATOR ELEMENTS and Assignee's U.S. Provisional Patent Application No. 60/759,778, filed Jan. 17, 2006, in the name of Hines, titled CONCENTRATING SOLAR PANEL AND RELATED SYSTEMS AND METHODS, which applications are incorporated herein by reference in their respective entireties for all purposes,. Such articulating concentrator systems desirably utilize a low overall height for the optical component, so that the concentrators can articulate freely.

As another drawback, parabolic troughs and dishes have aperture regions that are, in practice, unusable for concentrating. This is true for troughs and dishes that have either a bottom focus or an inverted focus. Portions of the apertures of these optical elements are unusable because both the bottom and inverted focusing configurations can be affected by angle of incidence limits at the target focal plane. For example, according to Snell's law, rays striking the target at greater than a certain angle are reflected off the surface and are not absorbed.

FIG. 4 schematically illustrates this issue for a bottom focus reflector 34. Incident rays 36, 38, 40 are concentrated by reflector 34 onto focal plane 32. The angle of incidence with respect to the focal plane 32 of the concentrated rays is greater for rays closer to the optical axis (not shown), which extends through the middle of the reflector 34. Rays 36 and 38 impinge on focal plane 32 at angles less than the acceptance angle of the focal plane 32 and are absorbed. Ray 40 impinges on focal plane 32 at an angle greater than the acceptance angle of the focal plane and is reflected back out of the reflector 34 as ray 42. The same effect would be seen if ray 42 would be incident ray and ray 40 would be the rejected ray. The regions 44 and 46 associated with non-absorbed rays 44 and 42 define the portion of the reflector's 34 aperture that is not usable for concentrating. In practical effect, the effective aperture of the system is reduced.

Inverted focus reflectors suffer from a similar effect except that the aperture penalty occurs near the periphery of the reflector. As schematically illustrated in FIG. 5, incident rays 52, 56, 60 are concentrated by reflector 50 onto focal plane 48. In contrast to the situation with a bottom focus reflector, the angle of incidence with respect to the focal plane 48 of the reflector 50 increases as rays strike reflector 50 further away from the optical axis (not shown), which extends through the middle of the reflector. Rays 52 and 60 impinge on focal plane 48 at angles less than the acceptance angle of the focal plane 48 and are absorbed. Ray 56 impinges on focal plane 48 at an angle greater than the acceptance angle of the focal plane 48 and is reflected back out of the reflector 50 as ray 58. The same effect is seen if ray 58 would be the incident ray and ray 56 would be the rejected ray. The regions 54 and 62 of non-absorbed rays 54 and 62 define the portion of the reflector's aperture that is not usable for concentrating. In practical effect, this limits the width of the reflector's aperture. In addition, as is typical of inverted focus configurations, reflector 50 suffers from self-shadowing such that rays nearest to the optical axis in region 64 are blocked by the target at the focal plane 48 itself, further reducing the light-collecting efficiency of the system.

In addition, articulating concentrator systems desirably would include a means to power the articulating components, preferably using power generated by the device itself. Conventional optical designs can present challenges for photovoltaic devices that would like to use self-powered articulation to aim light concentrating components at the source of incident light, e.g., the sun. It is important that self-powered designs be able to capture and concentrate diffuse light to provide power when the light concentrating components are not aimed properly. Such devices may use bottom focus reflectors in order to provide sufficient optical paths for diffuse radiation to strike a solar cell located at the focal plane. However, as implemented conventionally, this design choice occurs at the expense of the aforementioned limitations of the bottom focus reflector. Devices that instead use inverted focus reflectors, on the other hand, generally provide only very limited optical paths for diffuse radiation to reach the target, as the target, e.g., a solar cell, is facing away from diffuse radiative sources. Also, the reflected field of view in the primary mirror tends to be very narrow. Consequently, inverted focus reflectors tend to collect little diffuse light. These conventional bottom focus and inverted focus reflectors are therefore not well-suited to self-powered systems.

A third type of concentrating primary, a reflective lens as described in Vasylyev, U.S. Pat. No. 6,971,756, includes reflective elements in the form of concentric rings or parallel slats arranged so that incident rays are focused like a lens. These primaries can provide large concentration ratios and may overcome angle of incidence issues present with parabolic troughs and dishes. However, these generally include multiple, precision aligned surfaces that may be cost-prohibitive for medium-scale applications. Additionally, in the case of a long parallel slat form, additional support structure may be required that would tend to create undesirable optical obscurations. Further, in a manner that is analogous to the limitations of a refractive Fresnel lens discussed above, such a design has a limited ability to collect and focus diffuse light to provide for self-powering.

Some attempts have been made in the prior art to improve upon these solutions by combining multiple optical elements into a single concentrator, e.g., as described by Habraken in U.S. Pat. Pub. No. 2004/0134531 and by Cobert in U.S. Pat. Pub. No. 2005/0067008. However, both of these approaches place the multiple optical elements in series, so that light is redirected by multiple elements before reaching the focus. The significant disadvantage of these approaches is that they incur the expense and optical losses of two separate, full-aperture optical elements.

SUMMARY OF THE INVENTION

The present invention provides numerous solutions helpful singly or in combination to overcome and/or alleviate one or more of the problems present in prior art concentrators through the use of a hybrid reflective/refractive optical component. In preferred embodiments, the present invention provides a light collecting and concentrating optical component that includes both refractive and reflective elements. The component is hybrid in the sense that each element handles light collection and focusing for different portions of an aperture of the optical component. At least a portion of the aperture uses a refractive element while another portion of the primary aperture uses a reflective element. Either the reflective and/or referactive elements can be imaging and/or nonimaging. Advantageously, this allows many benefits of both refractive and reflective elements to be realized while avoiding conventional drawbacks.

The optical components of the invention advantageously may serve as a compact, primary optical component for an optical concentrator, especially solar trough or dish concentrators, and more particularly solar trough or dish concentrators that are self-powered and/or articulate. The present invention is applicable to both line and point concentrator systems. For line concentrators the refractive and reflective elements may have a geometry that is symmetric in one direction. For point concentrators the refractive and reflective elements may have a geometry that is symmetric in two directions. In both cases, the direction of symmetry is across the aperture of the concentrator.

In particularly preferred embodiments of this invention, the refractive element of the hybrid optical component is included in a transparent cover that fits over the light receiving end of the reflective element. Such an arrangement offers the significant advantage that the complete concentration system may be protectively enclosed beneath the protective cover and within the walls of the reflector (e.g., reflective trough or dish).

In one aspect, the present invention relates to a hybrid, concentrating optical component. The component includes an aperture; a reflective optical element that collects and focuses light onto a first target for a first portion of the aperture; and a refractive optical element that collects and focuses light onto a second target for a second portion of the aperture.

In another aspect, the present invention relates to a method of making an optical concentrating component. A light reflecting element is provided that collects incident light from a first portion of an aperture and concentrates the light onto a target. A refractive element is provided that captures incident light from a second portion of the aperture and concentrates the light onto the target.

In another aspect, the present invention relates to a method of collecting and concentrating incident light. Light is collected from a first portion of an aperture and reflecting the light from said first portion onto a target. Light also is collected from a second portion of the aperture and refracting the light from said second portion onto the target.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 a is a cross section view of a hybrid optical component of the present invention.

FIG. 1 b is a perspective view of the hybrid optical component of FIG. 1 a.

FIG. 2 is a cross-section view of a Fresnel lens refractive concentrator of the prior art.

FIG. 3 is a cross section view of a compound parabolic concentrator of the prior art.

FIG. 4 is a cross section view of a bottom focus parabolic reflector of the prior art.

FIG. 5 is a cross section view of an inverted focus parabolic reflector of the prior art.

FIG. 6 is a cross section view of a faceted trough form of a hybrid optical component of the present invention.

FIG. 7 is a cross section view showing optical pathways for diffuse light in the hybrid optical component of FIG. 1 a.

FIG. 8 is a perspective view of a point concentrator incorporating a hybrid optic component of the present invention.

DETAILED DESCRIPTION OF PRESENTLY PREFERRED EMBODIMENT

The embodiments of the present invention described below are not intended to be exhaustive or to limit the invention to the precise forms disclosed in the following detailed description. Rather a purpose of the embodiments chosen and described is so that the appreciation and understanding by others skilled in the art of the principles and practices of the present invention can be facilitated.

FIGS. 1 a, 1 b, and 7 show one preferred embodiment of a hybrid primary optical component 1 of this invention. For purposes of illustration optical component 1 is in the form of a line concentrator. The full aperture 15 of component 1 spans the width (in the case of a line concentrator) or diameter (in the case of a point concentrator) of the light receiving end 11 of a reflective element in the form of a bottom focusing dish 6. The hybrid primary optical component 1 includes a cover 8 fitted onto light receiving end 11. Together, the cover 8 and dish 6 provide a protective housing for device components housed in the interior 16.

The reflective surface of dish 6 of the preferred embodiment is nearly parabolic in shape. However, the reflecting element, as an alternative, can use any appropriate reflecting surface including but not limited to surfaces having linear, parabolic, faceted, spherical, elliptical, or hyperbolic profiles.

The cover 8 includes a refractive element in the form of integral plano-convex lens 4 in a central region of cover 8 and transparent, light transmissive outer regions 17 and 18. The lens 4 and dish 6 share a common focal plane 2 and a common optical axis 14. Lens 4 is positioned so that lens 4 is centered about the optical axis 14 of the component 1. The nearly parabolic reflector dish 6 also is centered about the optical axis 14 of the system.

Lens 4 may be of any suitable type including Fresnel and standard types. Even though Fresnel lenses tend to be expensive and lossy, Fresnel lenses are commonly used because a standard lens of the required diameter would be too thick and would use too much expensive and/or heavy optical material. In contrast, the refractive element of the present invention provides concentration for only a fraction of the system aperture 15, thereby allowing a smaller-diameter and thus much thinner lens for the same concentration ratio, as compared to a much thicker, full-aperture lens. As such, the present invention may alternatively employ a standard lens for a range of system apertures that would traditionally require a Fresnel lens. For purposes of illustration, lens 4 is shown as a standard lens.

A comparison between FIG. 1 and FIG. 2 illustrates this advantage given concentrators with, for instance, a 10× geometric concentration in one dimension. Both primary optics (that is, the Fresnel lens primary optic 18 of FIG. 2 and the hybrid primary optical component 1 of FIG. 1 including lens 4 and reflecting dish 6) with normalized apertures of ten (10) units concentrate incident rays 10 and 20, respectively, onto focal planes 2 and 16, respectively, each having a normalized width of one (1) unit. The standard lens element 4 of the hybrid optics of FIG. 1 concentrates a fraction of the total aperture 15 in contrast to the Fresnel lens 18 of FIG. 2, which concentrates the entire aperture. In the hybrid optical component 1 of FIG. 1, the portion of the aperture not concentrated by lens 4 is concentrated by reflecting dish 6. Consequently, the embodiments of the present invention that use a standard, yet thin, standard lens 4 to concentrate only a portion of the aperture 15 may reduce the system cost. In this regard, compare the large thick, full aperture, standard lens of Cobert, U.S. patent application Ser. No. 2005/0067008, to the much smaller and thinner lens 4 of FIG. 1. The hybrid optics approach of FIG. 1 also may improve optical throughput by eliminating the loss associated with discontinuities present with a full aperture Fresnel lens. Such losses are illustrated by the improperly refracted ray 22 in FIG. 2.

Advantageously, each optical element of the hybrid primary optical component 1, i.e., lens 4 and dish 6 in this embodiment, serves as the primary optic for its respective portion of the collecting aperture 15. This differentiates component 1 from and improves upon multi-stage concentrators that incorporate refractive and reflective components only in series.

For example, in use, incident rays 12 that are incident upon the central portion of the collecting aperture 15 pass through lens 4 of cover 8 and are thereby refractively focused by lens 4 onto the common focal plane 2. In the meantime, incident rays 10 that are incident upon the outer portions 17 and 18 of the collecting aperture 15 pass through cover 8 and are focused by the reflecting dish 6 onto the common focal plane 2. In other words, incident rays 12 are concentrated by lens 4 and not by the dish 6, while incident rays 10 are concentrated by the dish 6 and not by the lens 4.

The hybrid approach provides numerous advantages. First, CPC reflector concentrators in which only a reflector is provided to serve a full aperture, as shown in FIG. 3, tend to be too tall to be well suited to applications in which the concentrators must articulate within close proximity of one another. In contrast, as illustrated in FIG. 1, the present invention enables concentrator designs that have comparable concentrating power to a CPC design at lower height/width ratios, e.g., a height/width ratio of one (1), making the hybrid approach well suited to applications in which an array of concentrators must articulate within close proximity of one another.

As another advantage, the present invention requires no additional obscuring support structure. In contrast, the reflective lens of Vasylyev, U.S. Pat. No. 6,971,756 requires multiple precision aligned surfaces and support structures.

Hybrid optics of the present invention also are very compatible for use with self-powered, articulating optical concentrators, because the present invention provides sufficient paths for diffuse radiation to reach the focus plane 2. This is best seen in FIG. 7. Because the total aperture 15 of the hybrid optical component of the present invention is larger than the lens aperture, there exist optical paths not parallel to the optical axis 14, through the cover element 8, that neither strike the refractive element 4 nor the reflective dish 6. These optical paths allow diffuse radiation 72 to be directly absorbed by a solar cell located at the focal plane 2. This helps an articulating optical concentrator that includes the hybrid optical component to generate sufficient self-power to articulate itself even when not pointed at the sun. In contrast, inasmuch as full aperture Fresnel refractors typically allow only a small amount of diffuse light to reach the focal plane, full aperture Fresnel-refractor systems are generally not well suited to self-powering.

The use of hybrid optics in accordance with the present invention also avoids a key drawback conventionally associated with full aperture reflective components. If a reflective element is used by itself to serve a full aperture, as explained above with respect to FIGS. 3 and 4, the aperture would include regions associated with non-absorbed rays. These regions correspond to portions of the aperture that are not available for concentrating in a conventional system. Specifically, conventional bottom focus and inverted focus reflectors serving the full aperture tend to have a poor acceptance angle for incident light in certain regions of the aperture and, as a consequence, tend to be poorly suited to self-powering applications.

In contrast, the present invention overcomes the above limitations of both bottom and inverted focus reflectors by using refractive concentrating for the portions of the system aperture where the reflector is not suitable. Thus, the lens 4 of the hybrid optical component 1 of the present invention is positioned in those regions of aperture 15 to collect and concentrate corresponding incident light that otherwise would be unused. The full aperture 15 not only is used for collecting and focusing (a feat which is not accomplished with a full aperture reflective element used by itself), but also the optics can further capture diffuse light for self-powering (a feat which is not accomplished with a full aperture refractive element such as a lens). The ability to capture and concentrate light using the full aperture also helps self-powering performance. In practical effect, the hybrid approach provides the benefits of both a reflector and a refractor without the major drawbacks of either.

In one preferred embodiment, the cover 8 and lens 4 are 5 inches wide and may be constructed of acrylic or methacrylic, and the trough is 5 inches wide and 5 inches deep and may be constructed of high-reflectivity, aluminum sheet metal manufactured by Alanod under the trade name MIRO (distributed by Andrew Sabel, Inc., Ketchum, Id.). In the preferred embodiment of optical component 1 shown in FIGS. 1 a, 1 b, and 7, the hybrid optical component forms the primary optic for the concentrator system, and light redirected by the hybrid optical component 1 directly strikes the target surface at focal plane 2. In alternative forms of this invention, the light redirected by this primary optic optionally may be further redirected by additional optics, or may be redirected by one or more pre-primary optics prior to reaching this primary optic. For example, alternative embodiments may include additional optical elements (not shown) intended to help steer diffuse radiation 72 through the clear regions of the cover 8. As another option, reflectors could be added outside of the enclosed space of the concentrator module to help direct additional diffuse radiation through the clear regions of the cover 8 to the focal plane 2.

In another alternate form of this invention, the individual reflective or the refractive elements of the hybrid optical component may be replaced by multiple distinct individual elements, each focusing its own portion of the input aperture, by way of example, using a faceted refractive lens with a parabolic or faceted-parabolic reflector. For instance, another alternate form of an optical component 65 of the present invention uses two faceted but monolithic reflectors 66 and 68 illustrated in FIG. 6. Each reflector 66, 68 includes a plurality of facets 70, each having a continuous profile that may include but is not limited to linear, spherical, parabolic, elliptical, and hyperbolic profiles. Faceted reflectors are advantageous in that they are non-imaging and may be designed to concentrate light more evenly across the focal plane 2. As the reflective element is composed of two disjoint reflectors this also helps to eliminate reflector material in the portion of the component aperture that is concentrated by the refractive element 4, possibly reducing cost.

In accordance with a preferred mode of practice, the facet coordinates can be determined by a methodology that uses the following parameters:

    • Ycell—Half width of the target cell or focal plane
    • Ø—Acceptance half angle (radians). This is the angle relative to the optical axis in which incident rays are still concentrated onto the target surface.
    • Ymax—Half width of the reflector
    • Zmax—Reflector height relative to the target surface.

The solution for each facet coordinate is an iterative process that begins with the outermost coordinate defined by (Ymax, Zmax). The first step is to compute the facet slope such that the an incident ray impinging on the top of the facet at an angle of +Ø from the optical axis results in a reflected ray that impinges the cell at a position −Ycell. The second step is to solve for the (y,z) coordinate of the facet bottom using the facet slope previously computed such that an incident ray impinging at the facet bottom at the angle −Ø from the optical axis results in a reflected ray that impinges the cell at a position +Ycell. These two steps are then repeated for each facet using the bottom (y,z) coordinate of the previous facet as the top coordinate of the next facet. The equations for these two steps are as follows:

m i = tan ( π - arc tan ( y i - y i = z i ) + ϕ 2 ) 1 )

Where: yi =−Ycell and mi is the slope of the facet whose top coordinate is (yi,zi).

y i = y i + + ( z i - 1 - m i - 1 y i - 1 ) tan ( π - 2 arc tan ( m i - 1 ) - ϕ ) 1 - m i - 1 tan ( π - 2 arc tan ( m i - 1 ) - ϕ ) 2 )

Where: yi +=Ycell

The following coordinates for a representative, faceted reflector can therefore be determined given:

Ycell=0.25″

Ø=2.1 degrees

(y0,z0)=(2.5″,5″)

Facet # y (in) z (in) m
1 2.5 5 4.212103
2 2.45662 4.817277 4.128815
3 2.400028 4.583623 4.020582
4 2.326947 4.289793 3.881534
5 2.233829 3.92835 3.705591
6 2.117269 3.496428 3.487403
7 1.974757 2.999432 3.223974
8 1.80587 2.454945 2.917091
9 1.613921 1.895013 2.576414
10 1.407809 1.363981 2.222312
11 1.20313 0.909121 1.885937

FIG. 8 shows another embodiment of a hybrid optical component 80 of the present invention that is in the form of a point concentrator. Component 80 includes a generally parabolic reflector dish 82 having light receiving end 84. Light transmissive cover 86 is fitted over light receiving end 84 and includes a light refractive element in a central region in the form of lens 88. Lens 88 is integral with cover 86. The dish 82 and lens 88 share a common focal point 90. In use, incident light rays 92 that impinge upon lens 88 are refracted and concentrated onto focal point 90. In the meantime, incident light rays 94 pass through cover 86 and are then reflectively concentrated by dish 82 onto the common focal point 90. Thus, dish 82 and lens 88 serve different portions of the full aperture of hybrid optical component 80.

All cited patents and patent publications are incorporated herein by reference in their respective entireties for all purposes.

Other embodiments of this invention will be apparent to those skilled in the art upon consideration of this specification or from practice of the invention disclosed herein. Various omissions, modifications, and changes to the principles and embodiments described herein may be made by one skilled in the art without departing from the true scope and spirit of the invention which is indicated by the following claims.

Patent Citations
Cited PatentFiling datePublication dateApplicantTitle
US3388739Sep 7, 1965Jun 18, 1968Donald M. OlsonHeat dissipator
US3957031May 29, 1975May 18, 1976The United States Of America As Represented By The United States Energy Research And Development AdministrationLight collectors in cylindrical geometry
US4000734Nov 6, 1975Jan 4, 1977Matlock William CSolar energy converter
US4002499Jul 26, 1974Jan 11, 1977The United States Of America As Represented By The United States Energy Research And Development AdministrationRadiant energy collector
US4003638Sep 15, 1975Jan 18, 1977The University Of ChicagoRadiant energy collection
US4022186Sep 10, 1975May 10, 1977Northrup Jr Leonard LCompound lens solar energy system
US4067764Mar 15, 1977Jan 10, 1978Sierracin CorporationThermoplastic layers
US4069812Dec 20, 1976Jan 24, 1978E-Systems, Inc.Solar concentrator and energy collection system
US4092531Nov 16, 1976May 30, 1978Hughes Aircraft CompanyImmersed reflector quadrant detector
US4107521Oct 14, 1976Aug 15, 1978Gordon Robert WindersSolar sensor and tracker apparatus
US4131485Mar 6, 1978Dec 26, 1978Motorola, Inc.Conic reflector surfaces, conversion to electricity
US4146785Feb 13, 1978Mar 27, 1979Sunpower Systems CorporationSun-tracking control system for solar collector
US4158356Feb 22, 1977Jun 19, 1979Wininger David VSelf-powered tracking solar collector
US4168696Sep 30, 1976Sep 25, 1979Kelly Donald AFour quadrant, two dimensional, linear solar concentration panels
US4169738Nov 21, 1977Oct 2, 1979Antonio LuqueDouble-sided solar cell with self-refrigerating concentrator
US4177083Sep 6, 1977Dec 4, 1979Acurex CorporationPhotovoltaic concentrator
US4184482Sep 29, 1978Jan 22, 1980Cohen ElieSolar energy collecting system
US4187123Nov 15, 1977Feb 5, 1980Diggs Richard EDirectionally controlled array of solar power units
US4191164 *Oct 20, 1976Mar 4, 1980Kelly Donald ADual conversion steam and electric solar power system
US4210121Jun 15, 1977Jul 1, 1980Virgil StarkSolar energy collection
US4211212Dec 29, 1978Jul 8, 1980Braun Raymond JSolar refrigeration system
US4215410Feb 9, 1979Jul 29, 1980Jerome H. WeslowSolar tracker
US4223174Jul 19, 1976Sep 16, 1980Sun Trac CorporationSun-tracking solar energy conversion system
US4238246Jun 4, 1979Dec 9, 1980North American Utility Construction Corp.Solar energy system with composite concentrating lenses
US4253880Sep 5, 1978Mar 3, 1981U.S. Philips CorporationDevice for the conversion of solar energy into electrical energy
US4256364Feb 13, 1979Mar 17, 1981Canon Kabushiki KaishaTwo-dimensional scanning optical system with distortion correction
US4262195Jul 25, 1979Apr 14, 1981The United States Of America As Represented By The Administrator Of The National Aeronautics And Space AdministrationSolar tracking system
US4269168Dec 18, 1978May 26, 1981Johnson Steven AFocusing reflector solar energy collector apparatus and method
US4280853Mar 24, 1980Jul 28, 1981Centro Ricerche Fiat S.P.A.Solar energy conversion unit
US4287411Jun 19, 1979Sep 1, 1981Gori & Zucchi S.P.A.Apparatus for seeking and following a luminous zone, such as the sun
US4296731Jun 1, 1978Oct 27, 1981Cluff C BrentTracking booster and multiple mirror concentrator floating collector
US4297521Dec 18, 1978Oct 27, 1981Johnson Steven AFocusing cover solar energy collector apparatus
US4307711Feb 25, 1980Dec 29, 1981Doundoulakis George JSun tracking solar energy collector system
US4320288Apr 25, 1980Mar 16, 1982Thermo Electron CorporationSolar tracking system
US4323052Jun 4, 1979Apr 6, 1982Virgil StarkSolar energy system
US4328789Sep 24, 1979May 11, 1982American SolarSolar tracking drive mechanism
US4349733Jul 3, 1980Sep 14, 1982Beam Engineering, Inc.Sun tracker
US4354484Jan 5, 1981Oct 19, 1982Transolar, Inc.Solar collection system
US4365617Oct 2, 1980Dec 28, 1982Eckhard BugashSolar energy heating system
US4397303Feb 9, 1981Aug 9, 1983Armco Inc.Heat exchanger for concentrating solar collectors and method for making the heat exchanger
US4398053Feb 9, 1981Aug 9, 1983Orillion Alfred GPyramidal energy collector
US4410757Mar 22, 1982Oct 18, 1983Monegon, Ltd.Adjustable collection members for solar energy systems
US4459972Oct 6, 1981Jul 17, 1984Veda IncorporatedHeliostat assembly
US4476854Nov 14, 1983Oct 16, 1984Zomeworks CorporationGas spring solar tracker
US4484334Nov 17, 1981Nov 20, 1984Allied CorporationOptical beam concentrator
US4495408May 7, 1982Jan 22, 1985Kei MoriSunlight direction sensor
US4554038Aug 29, 1980Nov 19, 1985Trw Inc.Process for fabricating lightweight, rigid solar array substrate
US4556788Nov 17, 1983Dec 3, 1985Rca CorporationAmorphous silicon cell array powered solar tracking apparatus
US4572161Jun 18, 1984Feb 25, 1986Kei MoriSolar ray collector device
US4575639Dec 16, 1980Mar 11, 1986Rogow Bruce IFluid turbine system
US4601282Jul 12, 1984Jul 22, 1986Total Solar Energy Systems, Inc.Automatic solar collector system
US4604494Nov 7, 1984Aug 5, 1986General Electric CompanyPhotovoltaic cell array with light concentrating reflectors
US4619244Feb 17, 1984Oct 28, 1986Marks Alvin MSolar heater with cavity and phase-change material
US4622470Apr 16, 1984Nov 11, 1986Rca CorporationShutter control system
US4750943Oct 27, 1986Jun 14, 1988Tpv Energy Systems, Inc.Thermophotovoltaic system
US4771764Apr 6, 1984Sep 20, 1988Cluff C BrentHeat exchange means
US4868379Jun 20, 1988Sep 19, 1989Utility Power GroupPhotovoltaic array with two-axis power maximization tracking
US4945731Dec 12, 1988Aug 7, 1990Parker Robin ZAbsorbing fluid receiver for solar dynamic power generation and solar dynamic power system
US4968355Apr 14, 1989Nov 6, 1990Johnson Kenneth CTwo-axis tracking solar collector mechanism
US4995377Jun 29, 1990Feb 26, 1991Eiden Glenn EDual axis solar collector assembly
US4999483Dec 12, 1989Mar 12, 1991Kabushiki Kaisha ToshibaSensor for detecting two dimensional angle of incidence of the sun
US5255666Oct 13, 1988Oct 26, 1993Curchod Donald BSolar electric conversion unit and system
US5317145Apr 30, 1993May 31, 1994Wattsun CorporationRadiation source detector and tracker control having a shade pole and radiation responsive surface in the shape of narrow bands
US5483060Aug 17, 1993Jan 9, 1996Nippondenso Co., Ltd.Optical position sensor and isolation sensor using this position sensor
US5498297Sep 15, 1994Mar 12, 1996Entech, Inc.Photovoltaic receiver
US5665174Feb 16, 1993Sep 9, 1997Laing; Johannes NikolausPlatform for recovering solar energy
US5727585Jun 24, 1995Mar 17, 1998Daume; JochenDevice for obtaining energy from sunlight with at least one solar collector
US5806955Jun 7, 1995Sep 15, 1998Tir Technologies, Inc.TIR lens for waveguide injection
US5977475Oct 10, 1997Nov 2, 1999Toyota Jidosha Kabushiki KaishaConverging solar module
US6020554Mar 19, 1999Feb 1, 2000Photovoltaics International, LlcTracking solar energy conversion unit adapted for field assembly
US6058930Apr 21, 1999May 9, 2000Shingleton; JeffersonSolar collector and tracker arrangement
US6079408Mar 26, 1999Jun 27, 2000Honda Giken Kogyo Kabushiki KaishaSun-ray tracking system
US6087646Jun 30, 1998Jul 11, 2000Hughes Electronics CorporationWide field-of-view radiation sensors and methods
US6089224Dec 8, 1997Jul 18, 2000Poulek; VladislavApparatus for orientation of solar radiation collectors
US6113342Aug 12, 1998Sep 5, 2000Long-Airdox CompanySelf-aligning battery changing system for electric battery-powered vehicles
US6127620Sep 3, 1997Oct 3, 2000Toyota Jidosha Kabushiki KaishaConverging solar module
US6498290May 29, 2001Dec 24, 2002The Sun Trust, L.L.C.Conversion of solar energy
US6531653Sep 11, 2001Mar 11, 2003The Boeing CompanyLow cost high solar flux photovoltaic concentrator receiver
US6620995Mar 28, 2002Sep 16, 2003Sergiy Victorovich VasylyevNon-imaging system for radiant energy flux transformation
US6680693Mar 7, 2002Jan 20, 2004The University Of Southern MississippiMethod and apparatus for automatically tracking the sun with an object
US6691701Aug 6, 2002Feb 17, 2004Karl Frederic RothModular solar radiation collection and distribution system
US6700054Jan 29, 2001Mar 2, 2004Sunbear Technologies, LlcRefractive interface and reflector; integrated with photovoltaic, photohydrolytic, heat engine, light pipe, or photothermal device
US6717045Oct 23, 2001Apr 6, 2004Leon L. C. ChenPhotovoltaic array module design for solar electric power generation systems
US6809413Apr 23, 2003Oct 26, 2004Sandia CorporationMicroelectronic device package with an integral window mounted in a recessed lip
US6843573Apr 28, 2003Jan 18, 2005Mario RabinowitzMini-optics solar energy concentrator
US6848442Jan 29, 2001Feb 1, 2005Michael B. HaberSolar panel tilt mechanism
US6870087Sep 16, 2002Mar 22, 2005Patrick GallagherAssembly method and apparatus for photovoltaic module
US6881893Jun 10, 2003Apr 19, 2005David M. CobertSolar energy collection system
US6903261May 17, 2002Jun 7, 2005Universite De LiegeSolar concentrator
US6959993Jul 9, 2004Nov 1, 2005Energy Innovations, Inc.Solar concentrator array with individually adjustable elements
US6963437Sep 11, 2003Nov 8, 2005Gentex CorporationA package for encapsulating an integrated circuit optical sensor includes an electrochromic element having a transmittance that varies in response to an electrical signal; image recorder for recording a scene or object; cameras
US6971756Dec 17, 2001Dec 6, 2005Svv Technology Innovations, Inc.Apparatus for collecting and converting radiant energy
US7055519Dec 10, 2003Jun 6, 2006United Technologies CorporationSolar collector and method
US7076965Mar 28, 2002Jul 18, 2006John Beavis LasichCooling circuit for receiver of solar radiation
US7109461Mar 28, 2002Sep 19, 2006Solar Systems Pty Ltd.Solar tracking system
US7156088Jun 2, 2005Jan 2, 2007Energy Innovations, Inc.Solar collector mounting array
US7188964Dec 8, 2003Mar 13, 2007Xinetics, Inc.Integrated actuator meniscus mirror
US7192146Jul 28, 2004Mar 20, 2007Energy Innovations, Inc.Solar concentrator array with grouped adjustable elements
US7218998Jul 11, 2005May 15, 2007Neale Stephen DSystem and method for limiting power demand in an energy delivery system
US7388146Aug 2, 2002Jun 17, 2008Jx Crystals Inc.Planar solar concentrator power module
US7403278 *May 29, 2007Jul 22, 2008Shibaura Mechatronics CorporationSurface inspection apparatus and surface inspection method
Non-Patent Citations
Reference
1Burge et al., "Lightweight Mirror Technology Using a Thin Facesheet With Active Rigid Support," Proc. SPIE 3356, Space Telescopes and Instruments V, pp. 690-701, 1998.
2Cho et al., "Optimization of the ATST Primary Mirror Support System," Proc. SPIE 6273, Optomechanical Technologies for Astronomy, 2006.
3http://www.nrel.gov/docs/fy99osti/25410.pdf(Kurtz et al., "Concentrator and Space Applications of High-Efficiency Solar Cells-Recent Developments," Presented at the National Center for Photovoltaics Program Review Meeting, Denver, Colorado, Sep. 1998) 9 pages.
4http://www.nrel.gov/docs/fy99osti/25410.pdf(Kurtz et al., "Concentrator and Space Applications of High-Efficiency Solar Cells—Recent Developments," Presented at the National Center for Photovoltaics Program Review Meeting, Denver, Colorado, Sep. 1998) 9 pages.
5Kurtz and Friedman, "Photovoltaics-Lighting the Way to a Brighter Future," Optics & Photons News, pp. 30-35, Jun. 2005.
6Prisms & Flats from Pacific Rim Optical, Inc., http://www.krugeroptical.com/pro-prisms.asp, copyright 2009, 1 page.
7Prisms & Flats from Pacific Rim Optical, Inc., http://www.krugeroptical.com/pro—prisms.asp, copyright 2009, 1 page.
8Richman, R.H. et al., "Investigation of high-concentration photovoltaic cell packages after three years field service," Solar Energy Materials and Solar Cells 30, No. 3, pp. 263-276, Aug. 1993.
9Swanson, "The Promise of Concentrators," Prog. Photovolt. Res. Appl., vol. 8, pp. 93-111 (2000).
Referenced by
Citing PatentFiling datePublication dateApplicantTitle
WO2013032954A1 *Aug 24, 2012Mar 7, 2013Joseph John RHigh speed free-space optical communications
Classifications
U.S. Classification359/726, 126/689, 359/727
International ClassificationG02B17/00
Cooperative ClassificationG02B19/0042, G02B19/0028, H01L31/0522, F24J2/08, Y02E10/44, F24J2/06, Y02E10/52, F24J2/14, Y02E10/42, F24J2/085, G02B3/08, Y02E10/45, F24J2/12
European ClassificationH01L31/052B, F24J2/12, F24J2/08, G02B17/08N3, F24J2/14, G02B3/08, F24J2/06
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